Check force on energy

It is common practise to use the potential energy as a collective energy. Some MD codes thus pass the potential energy to PLUMED and PLUMED can then apply forces on this collective variable. We test that any forces that PLUMED applies on the potential energy are correctly passed back to the MD code by doing the following test. We first run a short simulation at $T$ K with a timestep of $\tau$ ps. During the course of this simulation we monitor the potential energy using the following PLUMED input:

Click on the labels of the actions for more information on what each action computes
tested on2.10
tested onmaster
e: ENERGYCalculate the total potential energy of the simulation box. More details
v: VOLUMECalculate the volume the simulation box. More details
PRINTPrint quantities to a file. More details ARGthe labels of the values that you would like to print to the file=e,v FILEthe name of the file on which to output these quantities=energy1

We then run a second simulation (starting from identical conditions) at a temperature of $T\alpha$ and with a timestep of $\tau/\sqrt(\alpha)$. The thermostat and barostat relaxation times are similarly divided by $\sqrt(\alpha)$. In the tests that are run on this website we set $\sqrt(\alpha)=1.1$. The PLUMED file above is used when this test is run but a different time series of energy values is recorded as the MD parameters in this second simulation are different.

If PLUMED is working correctly we should be able to recapture the time series of energy values for the first simulation by running an MD simulation with the modified parameters that were used in the second simulation and the following PLUMED input file:

Click on the labels of the actions for more information on what each action computes
tested on2.10
tested onmaster
e: ENERGYCalculate the total potential energy of the simulation box. More details
v: VOLUMECalculate the volume the simulation box. More details
# slope is such that 
PRINTPrint quantities to a file. More details ARGthe labels of the values that you would like to print to the file=e FILEthe name of the file on which to output these quantities=energy2
# slope should be (alpha-1)=0.21
RESTRAINTAdds harmonic and/or linear restraints on one or more variables. More details ATthe position of the restraint=0.0 ARGthe values the harmonic restraint acts upon=e SLOPE specifies that the restraint is linear and what the values of the force constants on each of the variables are=0.21

In other words, when forces are passed correctly the time series for the energies and volumes from the first and third of these calculations should be identical.

To determine if PLUMED passes this test we calculate the difference between the time series that were observed in the first and third simulations described above. We then divide this by the difference between the first and second time series.

An NPT version of this calculation is performed as well as an NVT calculation if the virial is passed to PLUMED.

Trajectories

  1. Input and output files for the unpeturbed calculation are available in this zip archive

  2. Input and output files for the peturbed calculation are available in this zip archive

  3. Input and output files for the peturbed calculation in which a PLUMED restraint is used to undo the effect of the changed MD parameters are available in this zip archive

Results

Original With PLUMED Effect of peturbation % Difference
-18174.8223 11.6346 -18174.8223 11.6346 0.0000 0.0000 0.0000 0.0000
-18171.8203 11.6346 -18193.2891 11.6346 6.8730 0.0000 312.3615 0.0000
-18196.7891 11.6475 -18234.4922 11.6321 25.0508 0.0054 150.5068 284.9140
-18174.7461 11.6475 -18289.0938 11.6321 26.6641 0.0054 428.8456 284.9140
-18168.7793 11.6475 -18331.0371 11.6321 36.6133 0.0054 443.1665 284.9140
-18157.8223 11.6475 -18356.3555 11.6321 44.8320 0.0054 442.8378 284.9140
-18146.1582 11.6475 -18364.7266 11.6321 51.8730 0.0054 421.3525 284.9140
-18138.9297 11.6475 -18362.1113 11.6321 58.5449 0.0054 381.2143 284.9140
-18139.2969 11.6475 -18356.5430 11.6321 64.7832 0.0054 335.3432 284.9140
-18146.6699 11.6475 -18353.7520 11.6321 69.2969 0.0054 298.8331 284.9140
-18157.1465 11.6475 -18355.4805 11.6321 70.4512 0.0054 281.5198 284.9140
-18166.0664 11.6475 -18360.2852 11.6321 67.7363 0.0054 286.7276 284.9140
-18171.4883 11.6475 -18366.7227 11.6321 63.5098 0.0054 307.4084 284.9140
-18176.2109 11.6475 -18375.6660 11.6321 62.5371 0.0054 318.9388 284.9140
-18185.8789 11.6475 -18389.7812 11.6321 68.6992 0.0054 296.8045 284.9140
-18203.8828 11.6475 -18410.0176 11.6321 80.8730 0.0054 254.8869 284.9140
-18227.0215 11.6475 -18432.2578 11.6321 91.6777 0.0054 223.8671 284.9140
-18246.4453 11.6475 -18448.2871 11.6321 91.9258 0.0054 219.5704 284.9140
-18253.2617 11.6475 -18451.0156 11.6321 77.4941 0.0054 255.1856 284.9140
-18244.2754 11.6475 -18439.2812 11.6321 52.7559 0.0054 369.6383 284.9140

The table below includes some of the results from the calculation. The columns contain:

  1. Time series for the energy and volume that were obtained from the simulation at $T$ K, $x_{md}$.
  2. Time series for the energy and volume that were obtained from the simulation at $\alpha T$ K and in which PLUMED applied a restraint on the energy, $x_{pl}$.
  3. The absolute value of the difference between the time series of energies and volumes that were obtained from the simulations running at $T$ K and $\alpha T$ K, $\vert x_{md}’-x_{md} \vert$. No PLUMED restraints were applied in either of these simulations.
  4. The values of $100\frac{\vert x_{md} - x_{pl}\vert }{ \vert x_{md}’-x_{md} \vert}$.

If the PLUMED interface is working correctly the first two sets of numbers should be identical and the final column should be filled with zeros.

Graphical representation (beta)

A visualization of the table above:
engvir_v2.10